Our proposed architecture is well-suited to accommodate modifications to these general steps. The different layouts for the magic state factories, the data and the ancilla blocks, and the boundary conditions of the data patches can be easily modified by an appropriate selection of the homodyne measurement quadratures. Note that as long as the fraction of swap-outs is below a critical value (which depends on the squeezing \(\Delta \) ), the general structure of our computing scheme carries through in the presence of swap-outs: both the GKP states in the lattice and \(p\) -squeezed states encode \(\left|+\right\rangle \)  and act appropriately under the physical operations we discussed [1]}. However, the swapped-out nodes add correlated noise to their neighborhood, an effect we deal with in the error-correction procedure, which we address in the following section.
